JPS60222748A - Method and apparatus for measuring specific gravity - Google Patents
Method and apparatus for measuring specific gravityInfo
- Publication number
- JPS60222748A JPS60222748A JP7858184A JP7858184A JPS60222748A JP S60222748 A JPS60222748 A JP S60222748A JP 7858184 A JP7858184 A JP 7858184A JP 7858184 A JP7858184 A JP 7858184A JP S60222748 A JPS60222748 A JP S60222748A
- Authority
- JP
- Japan
- Prior art keywords
- specific gravity
- body fluid
- circuit
- ultrasonic
- temp
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N29/00—Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
- G01N29/02—Analysing fluids
- G01N29/024—Analysing fluids by measuring propagation velocity or propagation time of acoustic waves
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N9/00—Investigating density or specific gravity of materials; Analysing materials by determining density or specific gravity
- G01N9/24—Investigating density or specific gravity of materials; Analysing materials by determining density or specific gravity by observing the transmission of wave or particle radiation through the material
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2291/00—Indexing codes associated with group G01N29/00
- G01N2291/02—Indexing codes associated with the analysed material
- G01N2291/028—Material parameters
- G01N2291/02818—Density, viscosity
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2291/00—Indexing codes associated with group G01N29/00
- G01N2291/02—Indexing codes associated with the analysed material
- G01N2291/028—Material parameters
- G01N2291/02881—Temperature
Landscapes
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Acoustics & Sound (AREA)
- Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、体液中の超音波伝播速度と体液の温度により
、体液の比重全算出する比重測定方法及びその装置に関
するものでめる。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a specific gravity measuring method and apparatus for calculating the total specific gravity of a body fluid based on the ultrasonic propagation velocity in the body fluid and the temperature of the body fluid.
従来、体液の比重全測定する方法としては、重量法や浮
秤法が用いられてきたが、体液、例えば、尿、血液、血
佑、血清等を大型に準備することを必要とし、また、連
続・定期的な測定には不便である。更に、尿比重等を測
定する方法として、屈折法も用いられているが、混濁床
及び、血液等の比重は測定できない欠点があった。Conventionally, the gravimetric method and floating scale method have been used to measure the total specific gravity of body fluids, but these methods require the preparation of large volumes of body fluids, such as urine, blood, blood, serum, etc. It is inconvenient for continuous and periodic measurements. Furthermore, the refraction method is also used as a method for measuring urine specific gravity, etc., but it has the drawback that it cannot measure the specific gravity of turbid beds and blood.
超音波の特注として、その伝播速度が浴液の成分及び温
度に依存することが知られている。体液の比重全測定す
る時、体液の温度は必ずしも一定ではなく、従来のよう
な溶液中の超音波伝播速度の変化によって比重全測定す
る装置(fllえば、特開昭57−108084号公報
)では温度の影響會受け、また、測定時に温度と溶液中
の超音波伝播速度との関係全演算処理する事ができない
為、正確な測定は難しいという欠点があった。また、超
音波食用いて標準溶液と被測定溶液との伝播速度の比較
による比重測定方法(特開昭54−60968号公報ン
があるが、標準溶液と被測定溶液との成分が非常に近い
ものに限られ、体液等の多種成分の混合清液では、標準
溶液との伝播速度の比較によって広範囲な比重を高精度
に測定することは録しいという欠点があった。As a customization of ultrasound, it is known that its propagation speed depends on the composition and temperature of the bath liquid. When measuring the total specific gravity of a body fluid, the temperature of the body fluid is not necessarily constant, and conventional devices that measure the total specific gravity by changing the ultrasonic propagation velocity in the solution (for example, Japanese Patent Application Laid-open No. 108084/1984) This method has the disadvantage that accurate measurement is difficult because it is affected by temperature and cannot perform all calculations on the relationship between temperature and ultrasonic propagation velocity in the solution during measurement. In addition, there is a method for measuring specific gravity by comparing the propagation speed of a standard solution and a solution to be measured using ultrasonic waves (Japanese Patent Application Laid-Open No. 54-60968). However, it is difficult to accurately measure a wide range of specific gravity by comparing the propagation velocity with a standard solution for mixed liquids containing various components such as body fluids.
本発明は、このような欠点に鑑み、超音波伝播速度が溶
液の成分及び温度に依存する原理に基づき、体液中の超
音波伝播速度及び体液の温度全直接測定し、その粘果會
もとに演算して体液の比重を測定する比重測定方法、及
び体液の比重を簡単且つ迅速に演算・算出する装置全提
供すること金目的としたものである。In view of these drawbacks, the present invention is based on the principle that the ultrasonic propagation velocity depends on the components and temperature of the solution, and the present invention directly measures the ultrasonic propagation velocity in body fluids and the temperature of the body fluid, and measures the viscous body of the fluid. The object of the present invention is to provide a specific gravity measuring method for measuring the specific gravity of a body fluid by calculating the specific gravity of the body fluid, and an apparatus for easily and quickly calculating and calculating the specific gravity of a body fluid.
即ち、本発明は、体液中に超音波を伝播させ、該超音波
伝播速度と該体液温度より演算して体液の比重を算出す
ることt#f徴とする比重測定方法、及び、体液内に支
持される超音波送受波器と一定の伝播距離を保って支持
される反射板により超音波全送受信させ、該体液中の超
音波伝播時間と伝播距離から超音波伝播速度全演算し、
該体液内の温度全温度センサーで測定し、超音波伝播速
度と体液温度よシ体液の比重全演算する回路ケ有した、
超音波食用いたことを%徴とする比重測定装置である。That is, the present invention provides a method for measuring specific gravity in which the specific gravity of a body fluid is calculated by propagating an ultrasonic wave into a body fluid and calculating from the ultrasound propagation velocity and the temperature of the body fluid; The entire ultrasonic wave is transmitted and received by a supported ultrasonic transducer and a reflecting plate that is supported while maintaining a constant propagation distance, and the entire ultrasonic propagation velocity is calculated from the ultrasonic propagation time and propagation distance in the body fluid,
It has a circuit that measures the total temperature within the body fluid with a temperature sensor and calculates the ultrasonic propagation velocity, body fluid temperature, and specific gravity of the body fluid.
This is a specific gravity measuring device that uses ultrasonic waves to measure the percentage of food consumed.
以下、図面等を参照して本発明の詳細な説明する。Hereinafter, the present invention will be described in detail with reference to the drawings and the like.
第1図は、本発明による装置のl実施例を示すブロック
図である。体液、例えば、尿、血液、血漿、血清等に、
超音波送受波器(4)と反射板(8)と温度センサー(
5)を組み込んだセンサー部(2)が浸されている。反
射板(8)と超音波送受波器t4Jとの間隔り。FIG. 1 is a block diagram illustrating an embodiment of a device according to the invention. In body fluids, such as urine, blood, plasma, serum, etc.
Ultrasonic transducer (4), reflector (8) and temperature sensor (
The sensor part (2) incorporating 5) is immersed. Distance between the reflector (8) and the ultrasonic transducer t4J.
は、センサー部(2)によって固定されていて、間隔L
oの2倍の2LOが超音波伝播距離となる。L。is fixed by the sensor part (2), and the interval L
2LO, which is twice o, is the ultrasonic propagation distance. L.
は、あらかじめLO設定器(6)に設定されている。is set in advance in the LO setting device (6).
つ
超音波回路は、シングアラウンド回路(8)で構成され
ておシ、第8図の(a)のように、超音波のパルス波(
20)が超音波送受波器(4)より体液(1円に送信さ
れ、反射板(8)にて反射し、再び超音波送受波器(4
)で、第8図(b)の超音波パルス波(21)が受信式
れる。次の超音波パルス波が送信されるまでの時間をτ
0(2B)とすると、受信後τo (2B)秒経過して
再び超音波送受波器(4)より第8図(alの超音波パ
ルス波(22)が送信される。第8図(c)のように送
信k n+1回(24)繰返した時間t (25)@測
定することで、体液中の超音波伝播速度v2下記の式で
計算する。The ultrasonic circuit consists of a sing-around circuit (8), and as shown in FIG. 8(a), the ultrasonic pulse wave (
20) is transmitted from the ultrasonic transducer (4) to the body fluid (1 circle), reflected by the reflecting plate (8), and transmitted again to the ultrasonic transducer (4).
), the ultrasonic pulse wave (21) shown in FIG. 8(b) is received. The time τ until the next ultrasonic pulse wave is transmitted
0 (2B), the ultrasonic pulse wave (22) in Fig. 8(al) is transmitted again from the ultrasonic transducer (4) after τo (2B) seconds have passed after reception. Fig. 8(c) ), the transmission k is repeated n+1 times (24) for a time t (25)@, and the ultrasonic propagation velocity in the body fluid v2 is calculated using the following formula.
V=(t−nτo) / (2n L(1)石は第1図
のτ0設定器(7)によって設定されている。V=(t-nτo)/(2n L(1) The stone is set by the τ0 setting device (7) in FIG.
シングアラウンド回路(8)より、超音波伝播速度Vの
情報、がゲート回路(113に通りCPU (12)に
入る。From the sing-around circuit (8), information on the ultrasonic propagation velocity V passes through the gate circuit (113) and enters the CPU (12).
第1図の温度センサー(5)の電圧変化を、温度測定回
路(9)によって温度情報に変換し、A//Dコンバー
ター回路(lO)でデジタル信号に変換し、ゲート回路
(ll)t−通り温度情報がCPU (12)に入る。The voltage change of the temperature sensor (5) in FIG. The temperature information enters the CPU (12).
本発明では記憶回路(18)に、体液中の温度■と超音
波伝播速度Mから体液の比重ヲ求める関数F(T、V)
の1例として多次多項式の定数を記憶させている。一般
に多次多項式は、
F=ΣaiTjVJ i * j、に;o−n)jk
で与えられる。この多次多項式の決定は、各溶液ごとに
行なわれている。多次多項式の1例の9元連立方程式
%式%
に各条件の温度、超音波伝播速度、重量法による比重を
代入して係数alt−求め、記憶回路(18)にatを
記憶させている。記憶回路(18)より係数ait−C
PU(12)が読み取り、温度情報と超音波伝播速度V
の情報を比重をめる関数F(T・V)に代入し、演算処
理を行なう。演算よりめられた比重値は、ゲート回路(
11)を通り、アンプ回路(l旬に入シ、表示回路(1
5)にて表示される。In the present invention, the memory circuit (18) stores a function F (T, V) for determining the specific gravity of the body fluid from the temperature (2) in the body fluid and the ultrasonic propagation velocity M.
As an example, constants of multi-dimensional polynomials are stored. In general, a multidimensional polynomial is given by: F=ΣaiTjVJ i * j, ;o−n)jk. This multidimensional polynomial is determined for each solution. The coefficient alt- is obtained by substituting the temperature, ultrasonic propagation velocity, and specific gravity according to the gravimetric method for each condition into the nine-dimensional simultaneous equation % formula, which is an example of a multidimensional polynomial, and at is stored in the memory circuit (18). . Coefficient ait-C from memory circuit (18)
PU (12) reads temperature information and ultrasonic propagation velocity V
The information is substituted into a function F(T·V) for weighting, and arithmetic processing is performed. The specific gravity value determined by the calculation is processed by the gate circuit (
11), enters the amplifier circuit (1), and the display circuit (1).
5) will be displayed.
本発明に従うと、体液の比重が連続且つ迅速に測定でき
る上に、従来の1童法、浮秤法に比べて簡単に測定でき
、屈折法では測定できなかった混濁法や血液等の体液の
比重も測定ができる。更に測定中の振動、温度の変動、
液の移動等の影響上次に、本発明の一例となる尿比重測
定値と、重量法による比重値との比較全行なう。別表1
に示した本発明による装置を用いて測定しfcJgの温
度と超音波伝播速度、及び重量法で測定した比重値のデ
ータより、係数aiをめた結果を別表2に示した。別表
8は不発明の装置を用いて測定しfc采比重の値と、重
量法で測定した値全列記したもので、本発明による比重
測定法が従来の重量法による比重と一致していることを
示している。According to the present invention, the specific gravity of body fluids can be measured continuously and quickly, and can be measured more easily than the conventional one-child method and floating scale method. Specific gravity can also be measured. Furthermore, vibrations and temperature fluctuations during measurement,
Due to the influence of liquid movement, etc., next, a complete comparison will be made between the urine specific gravity measured value, which is an example of the present invention, and the specific gravity value determined by the gravimetric method. Attached table 1
Table 2 shows the results of calculating the coefficient ai from the data of the fcJg temperature and ultrasonic propagation velocity measured using the apparatus according to the present invention shown in , and the specific gravity value measured by the gravimetric method. Attached Table 8 lists all the values of fc kettle specific gravity measured using an uninvented device and the values measured by the gravimetric method, and shows that the specific gravity measurement method according to the present invention is consistent with the specific gravity determined by the conventional gravimetric method. It shows.
以下、図面に従って1実施例を説明する。 One embodiment will be described below with reference to the drawings.
第2図は、センサー部(2)を示したものであり、セン
サー部(27を体液の中へ没す。ケーブル(16)?通
って電気信号が送られ、超音波送受波器(4) 、Cり
超音波が送信され、反射板(8)で反射され、超音波送
受波器(旬で受信され、ケーブル(16)f!:電気信
号、とじて送られる。超音波送受波器(4)は、保持具
(I8)によって反射板(8)との距離を一定に保たれ
、ケーブル(16)はケーブル押え(17)によって固
定されている。第2図(b)において保持具(18)は
、超音波送受波器(4)と反射板(8)全支持する部分
と、ケーブル(16ンに近接する保持部(19)とが角
度を有する屈曲形保持具である。第2図(clは、第2
図(a)のA−Aの断面よp超音波送受波器t4)の方
向を見た図であシ、温度センサー(5)は、保持具(1
8)に組み込まれている。Figure 2 shows the sensor unit (2), where the sensor unit (27) is immersed in body fluid.An electrical signal is sent through the cable (16) and the ultrasonic transducer (4). ,C ultrasonic waves are transmitted, reflected by the reflecting plate (8), received by the ultrasonic transducer (16), and sent to the cable (16) f!: electric signal.Ultrasonic transducer ( 4) is kept at a constant distance from the reflecting plate (8) by a holder (I8), and the cable (16) is fixed by a cable holder (17). 18) is a bent type holder in which the part that fully supports the ultrasonic transducer (4) and the reflection plate (8) and the holding part (19) close to the cable (16) are at an angle. Figure (cl is the second
This is a cross-sectional view taken along line A-A in Figure (a), looking in the direction of the ultrasonic transducer t4).
8).
別表1
※4℃の水に対する液温2θ℃の比重
別異2
別表8
※比重は、4°0の水に対する液温20“Cのものであ
る。Attached Table 1 *Differences by specific gravity of liquid temperature 2θ℃ relative to water at 4°C Attachment 8 *Specific gravity is for a liquid temperature of 20"C relative to water at 4°0.
第1図は、本発明による装置の実施例全示すプロッタ図
で、第2図(a)、第2図(blは、本発明による装置
で用いる超音波送受信部を示し、第2図fe)は、第2
図ta)のA−X断面↓り超音波送受波器の方向を見た
図で、温度センサーの実施例金示す。
第8図は、シングアラウンド方式全説明する為の図であ
る。
図中、(11は体液、(2)はセンサー部、(8)は反
射板、(4)は超音波送受波器、(8)はシングアラウ
ンド部、(勢は温度測定回路、(11)はゲート回路、
(12)はCPU(15)は表示回路・・・である。
特許出願人 住友ベークライト株式会社第1図
第2図
(a)
第3図
手続補正書(自発)
昭和59年11月7日
特許庁長官殿
1、事件の表示
昭和59年特許願第78581号
2、発明の名称
比重測定方法及びその装置
3、補正をする者
事件との関係 特許出願人
住 所 東京都千代田区内幸町1丁目2番2号明細書の
発明の詳細な説明の欄。
(1)明細書の第6頁第8行目
「a5V2」の後に、「+」を加入する。
以上FIG. 1 is a plotter diagram showing all the embodiments of the device according to the present invention, and FIG. 2(a) and FIG. is the second
This is a cross-sectional view taken along line A-X in Figure ta), looking in the direction of the ultrasonic transducer, showing an embodiment of the temperature sensor. FIG. 8 is a diagram for explaining the whole sing-around method. In the figure, (11 is a body fluid, (2) is a sensor part, (8) is a reflection plate, (4) is an ultrasonic transducer, (8) is a sing-around part, (is a temperature measurement circuit, (11) is is the gate circuit,
In (12), the CPU (15) is a display circuit. Patent applicant: Sumitomo Bakelite Co., Ltd. Figure 1 Figure 2 (a) Figure 3 Procedural amendment (voluntary) November 7, 1980 To the Commissioner of the Japan Patent Office 1 Indication of case 1989 Patent Application No. 78581 2 , Name of the invention Specific gravity measuring method and device 3, Relationship with the case of the person making the amendment Patent applicant address 1-2-2 Uchisaiwai-cho, Chiyoda-ku, Tokyo Column for detailed description of the invention. (1) Add "+" after "a5V2" on page 6, line 8 of the specification. that's all
Claims (1)
該体液温度より演算して該体液の比重全算出することを
特徴とする比重測定方法。 (2)体液内に支持されする超音波送受波器と一定の伝
播距離金保って支持される反射板により超音波全送受信
させ、該俸液申の超音波伝播時間と該伝播距離から談超
背波伝播速度を演算し、■体液内の温度全温度上ン丈−
で測定し、該超音波伝播速度と該体液温度より体液の比
重全演算する回路金有した、超音波音用いたことを特徴
とする比重測定装置。 (8)体液内に支持される超音波送受波器と一定の伝播
距離を保って支持される反射板全組み込んだ保持具にお
いて、該超音波送受波器と該反射板を支持丁ゐ部分と、
ケーブルに近接する保持部とが角度金有する屈曲形保持
具を特徴とする特許請求の範囲第2項記載の比重測定装
置。[Scope of Claims] (1) A method for measuring specific gravity, which comprises propagating ultrasonic waves into a body fluid and calculating the total specific gravity of the body fluid by calculating from the ultrasound propagation velocity and the temperature of the body fluid. (2) All ultrasonic waves are transmitted and received by an ultrasonic transducer supported in the body fluid and a reflector supported while maintaining a certain propagation distance, and the ultrasonic waves are estimated from the ultrasonic propagation time and propagation distance of the body fluid. Calculate the back wave propagation velocity and calculate the total temperature within the body fluid.
What is claimed is: 1. A specific gravity measuring device using ultrasonic sound, comprising a circuit for calculating the specific gravity of a body fluid from the ultrasonic propagation velocity and the temperature of the body fluid. (8) In a holder that incorporates an ultrasonic transducer supported in body fluid and a reflector supported at a constant propagation distance, the ultrasonic transducer and the reflector are connected to the supporting part. ,
3. The specific gravity measuring device according to claim 2, wherein the holding portion close to the cable is a bent holder having an angle bar.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7858184A JPS60222748A (en) | 1984-04-20 | 1984-04-20 | Method and apparatus for measuring specific gravity |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7858184A JPS60222748A (en) | 1984-04-20 | 1984-04-20 | Method and apparatus for measuring specific gravity |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS60222748A true JPS60222748A (en) | 1985-11-07 |
Family
ID=13665872
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP7858184A Pending JPS60222748A (en) | 1984-04-20 | 1984-04-20 | Method and apparatus for measuring specific gravity |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS60222748A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
BE1002682A3 (en) * | 1988-12-29 | 1991-04-30 | B & R Internat | Method and device for measuring at least one parameter of a fluid in a tank |
Citations (3)
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---|---|---|---|---|
JPS5460968A (en) * | 1977-10-24 | 1979-05-16 | Terumo Corp | Method and device for measuring liquid density by supersonic waves |
JPS56133644A (en) * | 1980-03-24 | 1981-10-19 | Toshiba Corp | Ultrasonic hydrometer |
JPS5877656A (en) * | 1981-11-04 | 1983-05-11 | Fuji Kogyo Kk | Ultrasonic measuring device for concentration |
-
1984
- 1984-04-20 JP JP7858184A patent/JPS60222748A/en active Pending
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5460968A (en) * | 1977-10-24 | 1979-05-16 | Terumo Corp | Method and device for measuring liquid density by supersonic waves |
JPS56133644A (en) * | 1980-03-24 | 1981-10-19 | Toshiba Corp | Ultrasonic hydrometer |
JPS5877656A (en) * | 1981-11-04 | 1983-05-11 | Fuji Kogyo Kk | Ultrasonic measuring device for concentration |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
BE1002682A3 (en) * | 1988-12-29 | 1991-04-30 | B & R Internat | Method and device for measuring at least one parameter of a fluid in a tank |
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